The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking

The fermionic sub-programme of Cosmochrony locates the three-generation mass split in the $J_3$-odd part of the squared projective endomorphism $E_\Pi^2$ restricted to the gauge-singlet generation triplet ${C^3_{\mathrm{gen}}}$, parametrised by a single real number $u$ through $E_\Pi^2|_{{C^3_{\mathrm{gen}}}}=\mathrm{diag}(1,\tfrac12+u,\tfrac12-u)$, with the even sector $\mathrm{diag}(1,\tfrac12,\tfrac12)$ already closed by Born–Infeld parity . This note fixes the structural status of $u$ before any explicit construction of $E_\Pi$. First, the projected Dirac square admits a universal Feshbach/Schur form $E_\Pi=-{\Pi_S}\,D\,(1-P)\,D\,{\Pi_S}^{*}=-M^{\dagger}M$ with $P={\Pi_S}^{*}{\Pi_S}$, exhibiting $E_\Pi$ as the Schur complement of the spinorial directions eliminated by the non-injective projection, negative semi-definite and vanishing in the injective limit. Second, the chiral block decomposition shows that $u$ is controlled by the ${\mathcal D}^{\pm}$-transported, generation-projected part of the antiunitary chiral equivariance defect \[ \Delta_\chi(P)=\pi_{LL}-\tau\,\overline{\pi_{RR}}\,\tau^{-1} \] of the eliminated block $1-P$, rather than by a naive block difference. Third, the minimal non-injectivity $c\leftrightarrow q-c$ is chirally symmetric, so $u=0$ at the level of axioms A1–A3; a non-zero $u$ requires a chiral symmetry-breaking that can originate only in the projection-locking axiom A4. The Seeley–DeWitt conventions are locked so that the operator-level and spectral-level definitions of $u$ coincide on the flat effective metric, and a no-go result establishes that $u$ is not accessible to any finite front observable because chirality is a Lorentzian rather than a finite-fibre datum. The remaining open deliverable is reduced to three sharp questions about A4.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-06-09
DOI
https://doi.org/10.5281/zenodo.20606280
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
preprint
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preprint

The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking

Jérôme Beau
Zenodo (CERN European Organization for Nuclear Research)
Quantum Chromodynamics and Particle Interactions
preprint

The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking

Jérôme Beau
preprint en

Abstract

The fermionic sub-programme of Cosmochrony locates the three-generation mass split in the $J_3$-odd part of the squared projective endomorphism $E_\Pi^2$ restricted to the gauge-singlet generation triplet ${C^3_{\mathrm{gen}}}$, parametrised by a single real number $u$ through $E_\Pi^2|_{{C^3_{\mathrm{gen}}}}=\mathrm{diag}(1,\tfrac12+u,\tfrac12-u)$, with the even sector $\mathrm{diag}(1,\tfrac12,\tfrac12)$ already closed by Born–Infeld parity . This note fixes the structural status of $u$ before any explicit construction of $E_\Pi$. First, the projected Dirac square admits a universal Feshbach/Schur form $E_\Pi=-{\Pi_S}\,D\,(1-P)\,D\,{\Pi_S}^{*}=-M^{\dagger}M$ with $P={\Pi_S}^{*}{\Pi_S}$, exhibiting $E_\Pi$ as the Schur complement of the spinorial directions eliminated by the non-injective projection, negative semi-definite and vanishing in the injective limit. Second, the chiral block decomposition shows that $u$ is controlled by the ${\mathcal D}^{\pm}$-transported, generation-projected part of the antiunitary chiral equivariance defect \[ \Delta_\chi(P)=\pi_{LL}-\tau\,\overline{\pi_{RR}}\,\tau^{-1} \] of the eliminated block $1-P$, rather than by a naive block difference. Third, the minimal non-injectivity $c\leftrightarrow q-c$ is chirally symmetric, so $u=0$ at the level of axioms A1–A3; a non-zero $u$ requires a chiral symmetry-breaking that can originate only in the projection-locking axiom A4. The Seeley–DeWitt conventions are locked so that the operator-level and spectral-level definitions of $u$ coincide on the flat effective metric, and a no-go result establishes that $u$ is not accessible to any finite front observable because chirality is a Lorentzian rather than a finite-fibre datum. The remaining open deliverable is reduced to three sharp questions about A4.

Zenodo (CERN European Organization for Nuclear Research)
Quantum Chromodynamics and Particle Interactions
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The Projective Residue as a Schur Complement: Reduction of the Generation Split to the Chiral Asymmetry of Projection Locking — Jérôme Beau · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS